This is the differential form of Faraday’s law of induction, one of Maxwell’s four equations. It states that a time-varying magnetic field ([latex]\mathbf{B}[/latex]) always accompanies a spatially varying, non-conservative electric field ([latex]\mathbf{E}[/latex]). The relationship is expressed as [latex]\nabla \times \mathbf{E} = -\frac{\partial \mathbf{B}}{\partial t}[/latex]. This equation governs how changing magnetic fields create electric fields at a specific point in space.
